1. Faculty of Materials Science and Chemical Engineering, Ningbo University, Ningbo 315201, China 2. Key Laboratory of Marine Materials and Related Technologies, Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, China
Cite this article:
Wentao LI,Zhenyu WANG,Dong ZHANG,Jianguo PAN,Peiling KE,Aiying WANG. Preparation of Ti2AlC Coating by the Combination of a Hybrid Cathode Arc/Magnetron Sputtering with Post-Annealing. Acta Metall Sin, 2019, 55(5): 647-656.
Nuclear power generation provides a reliable and economic supply of electricity, due to low carbon emissions and relatively few waste. However, the reaction between zirconium and steam at high temperature is accompanied by the release of large amounts of hydrogen gas, which will bring serious consequences. After the Fukushima nuclear accident, the concept of accident-tolerant fuels (ATF) has been proposed and widely investigated. In terms of nuclear claddings, one key requirement is reduced oxidation kinetics with high-temperature steam and hence significantly reduced heat and hydrogen generation. An economical and simple method could be the preparation of protective coatings on the surface of zirconium alloys to improve the oxidation resistance. The MAX phase has been considered to be one of the most promising coating materials for nuclear cladding coatings. In this work, Ti-Al-C coatings with different Ti/Al ratios have been deposited on Zirlo alloy using a hybrid arc/magnetron sputtering method, and the Ti2AlC coatings were obtained by post-annealing. The effects of Ti/Al ratios and annealing temperatures on the phase and microstructure of Ti-Al-C coatings after annealing were studied by SEM, EDS, XRD, Raman spectrometer and TEM. It is found that Ti-Al-C coatings with different Ti/Al ratios deposited by the hybrid cathode arc/magnetron sputtering are a multi-layer structure of an alternative Al-rich layer and TiCx layer. The as-deposited coatings are compact with a small amount of large particles. The Ti/Al ratio has an important influence on the phase structure of the annealed coating. When the Ti/Al ratio is 2.04, the highest purity and crystallinity of Ti2AlC are obtained. TiC and Ti3AlC impurities will form within the coating at a higher Ti/Al ratio (3.06), while the purity and crystallinity of Ti2AlC will decrease at a lower Ti/Al ratio (0.54). In addition, the annealing temperature affects the formation of Ti2AlC to a great extent. When the Ti/Al ratio is 2.38, the optimum temperature for Ti-Al-C coatings to Ti2AlC coatings is at 750 ℃. The atom cannot diffuse fully at a lower annealing temperature (600 ℃), which is difficult to form the Ti2AlC phase, while a higher annealing temperature (900 ℃) will enable the formation of Ti2AlC coatings with more TiC, TiAlx and other impurities.
Fund: National Science and Technology Major Project of China(2015ZX06004-001);China Postdoctoral Science Foundation(2018M632513);Natural Science Foundation of Zhejiang Province(LQ19E01002);Ningbo Municipal Key Technologies Research and Development Program(2017B10042)
Fig.1 Schematic of the hybrid cathodic arc/magnetron sputter (No.1~No.5 samples were suspended from top to bottom on a rotating sample holder in the chamber)
Procedure
Ar flow
mL·min-1
CH4 flow
mL·min-1
Presure
Pa
Bias voltage
V
Current / A
Ion gun
Arc
Sputter
Etching
40
-
-
-300
0.2
-
-
TiC layer
200
50
3.99
-100
-
70
-
Ti-Al-C layer
200
15
3.99
-200
-
60
8.0
Table 1 Deposition parameters of Ti-Al-C coatings
Sample
No.1
No.2
No.3
No.4
No.5
As-deposited
2.38
2.04
1.64
0.66
0.42
As-annealed
3.06
1.75
1.09
0.99
0.54
Table 2 Ti/Al ratios of No.1~No.5 coatings in as-deposited and annealed samples
Fig.2 Surface SEM images of No.1 (a), No.2 (b), No.3 (c), No.4 (d) and No.5 (e) coatings in as-deposited samples
Fig.3 Surface SEM images of No.1 (a), No.2 (b), No.3 (c), No.4 (d) and No.5 (e) coatings annealed at 800 ℃ for 1 h
Fig.4 Cross-sectional SEM images of No.1 (a), No.2 (b), No.3 (c), No.4 (d) and No.5 (e) coatings annealed at 800 ℃ for 1 h
Fig.5 EDS line-scanning and element mapping results of No.2 (a) and No.4 (b) samples annealed at 800 ℃ for 1 h
Fig.6 XRD spectra of the No.1~No.5 samples annealed at 800 ℃ for 1 h
Fig.7 Raman spectra of the as-deposited No.1 sample and the annealed one (E1g, E2g and A1g stand for three Raman active modes in MAX phase, respectively)
Fig.8 HRTEM images of as-deposited (a~c) and annealed (d, e) No.1 coatings, and fast Fourier transform image of area A in Fig.8e (f) (Illustration in Fig.8a shows selected-area electron diffraction pattern of as-deposited coating, and inset in Fig.8b shows line scan pattern of the coating surface under TEM, corresponding to the line)
Fig.9 Surface SEM images of No.1 sample as-deposited (a) and annealed at 600 ℃ (b), 650 ℃ (c), 700 ℃ (d), 750 ℃ (e), 800 ℃ (f), 850 ℃ (g) and 900 ℃ (h) for 1 h
Fig.10 Cross-section SEM images and EDS line-scanning results of No.1 sample as-deposited (a) and annealed at 600 ℃ (b), 650 ℃ (c), 700 ℃ (d), 750 ℃ (e), 800 ℃ (f), 850 ℃ (g) and 900 ℃ (h) for 1 h
Fig.11 XRD spectra of the No.1 sample annealed at 600~900 ℃ for 1 h
Fig.12 Raman spectra of the No.1 samples annealed at 600~900 ℃ for 1 h
Fig.13 Changes of grain size at (0002) and (10$\bar{1}$3) plane with different annealing temperatures for No.1 sample
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